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RV FRCERV=−
FR
Initial helium concentration)
Final helium concentration)
(
(
VV
F F
A
=−
8
7
Litres
Time
Total lung capacity
6
volume
5
4
3
2
1
0
Expiratory
reserve
volume
reserve
Inspiratory
Fig. 8.6 Normal adult lung volumes.
Tidal
volume
Residual
volume
CHAPTER 8 Respiratory System
capacity
Inspiratory
Functional residual
capacity
Vital
capacity
capacity
Expiratory
191
• residual volume (RVol): the volume remaining aer maximal expiration; it cannot be measured directly but can be estimated from other lung volumes:
• e anatomical dead space can be determined using Fowler’s method (Fig. 8.7). e subject breathes through a tube connected to a nitrogen analyser. e subject takes a single breath of pure oxygen, holds the breath for several seconds and then breathes out. By performing this manoeuvre the composition of air within the alveoli
• total lung capacity (TLC): the sum of all lung vol­umes plus the residual volume
• vital capacity (VC): the volume of air that is expelled from maximal inspiration to maximal expiration.
• Normal spirometry traces are shown in Fig. 8.6; they may vary for size, weight and gender.
• e FRC can be determined by the helium dilution method. e subject breathes normally from a spirom­eter lled with a known volume of air and helium. As the subject breathes in and out the helium is diluted in the air that is le in the lungs:
will dier from that within the airways (i.e. alveoli will contain nitrogen but airways higher up will have pure oxygen).
• Subject breathes out pure O2 (from conducting airways).
• As subject starts to expire, the nitrogen content of alveo­lar air is measured.
• A plot of exhaled volume to nitrogen concentration is produced; the dead space is the volume at the midpoint between nitrogen rst being detected and its plateau.
• Physiological dead space can be determined from the Bohr equation.
• e principles of this equation rely on two facts:
volume of spirometer
×
C
=
• all of the expired CO2 comes from the alveoli
• dead space is atmospheric air and thus has negligible
CO2 content.
• e RV can be calculated by the same method, but the subject takes a maximal expiration (i.e. only RV in the lungs) before breathing from the spirometer.
Dead Space and Alveolar Ventilation Rate
• Dead space is the volume of air which has to be venti­lated, but does not actually take part in gas exchange.
• Dead space can be anatomical or physiological:
• anatomical dead space is the volume of gas that does
not mix with the air in the alveoli
• physiological dead space is the volume of gas that
may reach the alveoli but, due to a lack of perfusion, does not take part in gas exchange (this includes air in the anatomical dead space).
• e Bohr equation is:
E
1
DE
VD: volume of dead space VE: volume of expired CO FE: fraction of expired CO FA: fraction of alveolar CO
FE can be measured simply by measuring the CO2 con-
2
2
2
tent of expired air.
FA can be measured from:
• the last part of the expired air, which will have the same composition as alveolar air
• arterial blood gas (more accurate).
192
V
V
D
=−
 
=
35
.
Alveolar ventilation rate TV dead space
=−
()
()
.
=
42 L/min
EXP
Vol. expired (mL)
% N
0
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SECTION II Physiology
100
2
50
200
Mid-point
150
100
Vol. of dead space
Fig. 8.7 Fowler’s method for determination of the anatomical dead space.
• For a normal subject with a tidal expiration of 500 mL, expired CO2 = 3.5% and alveolar CO2 = 5%; the dead space:
500 1
D
50
.
mL
500
• Factors that increase anatomical and physiological dead space are given in Table 8.2.
TABLE 8.2 Factors Increasing Anatomical
and Physiological Dead Space
Anatomical Dead Space
Increasing size of the subject Hypotension
Standing position Hypoventilation
Increased lung volume Emphysema
• Alveolar ventilation rate is the rate at which gas in the alveoli is replaced:
Respiratoryrate
×
()
=−×
500150 12
RR
Bronchodilatation Positive pressure
• Values will fall dramatically in respiratory disease; PEFR is particularly useful in assessing the severity of acute asthma attacks.
Peak Expiratory Flow Rate (PEFR)
• A simple bedside test of respiratory function.
• Patient is asked to take maximal inspiration and then to blow out as fast as possible into the peak ow meter.
• Values will vary for age, sex and weight, but a value of around 4–500 L/min is normal.
Closing Capacity
• is is the volume of the lungs at which small airways at the base of the lung start to close.
• e signicance of the closing capacity is that as air leaves the lungs some airways close and trap air in the
Physiological Dead Space
and PE
ventilation
CHAPTER 8 Respiratory System
Lung vol. (L)
100
1 2 3 4
2
% N
Closing capacity
TLC FRC CC RV
Fig. 8.8 The concentration of nitrogen following a single inspiration of 100% oxygen. The closing capacity is
indicated at the point of abrupt increase in the nitrogen concentration.
193
alveoli; these alveoli cannot play a full part in respira­tory gas exchange.
• Closing capacity can be measured by the following technique:
• the subject breathes out to residual volume and then
takes a maximal inspiration of 100% O
• the subject then takes a full expiration through a
2
nitrogen meter
• the plot of nitrogen concentration to lung volume
gives a characteristic plot with four phases (Fig. 8.8):
• phase 1: pure dead space is exhaled and is there­fore 100% O
• phase 2: mixture of dead space and alveolar gas
2
(nitrogen concentration from alveoli increases concentration)
• phase 3: pure alveolar gas (plateau phase)
• phase 4: abrupt increase in nitrogen concen­tration as airways at the base of the lung close. Expired air at this point is from the apex, which has received less O2, and thus the nitrogen is less dilute.
• Closing capacity is normally 10% of the vital capacity.
• Factors aecting the closing capacity include:
• age: increases with age
• posture: in a supine position in a 40-year-old subject, the closing capacity is equal to the FRC
• anaesthesia: decrease in lung volumes results in clos­ing capacity exceeding FRC, even in the youngest patients.
Flow–Volume and Volume–Time Curves
• Spirometry values should always be assessed with ow– volume and volume–time curves. Diseases of the lung produce characteristically shaped curves.
• Flow–volume curves (Fig. 8.9).
• Volume–time curves (Fig. 8.10).
Diffusion Capacity
• Diusion capacity (DLCO) or transfer factor (TLCO) is a test that reects both the diusion capacity of the alveo­lar membrane and also the pulmonary vasculature.
• It can be measured by inhaling very small concentra­tions of carbon monoxide and measuring the increase in arterial CO.
DLCO is reduced with:
in diusion distance, i.e. pulmonary oedema
• loss of alveolar area, i.e. emphysema.
PULMONARY BLOOD FLOW
Structure of the Lung
See Anatomy section (Chapter 1).
194
Vol (L)
Vol (L)
Flow (L/s)
TLC RV
Vol (L)
Volume
Time
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SECTION II Physiology
Flow (L/s)
Normal
Restrictive
Normal
Normal
A
Flow (L/s)
B
C
Fig. 8.9 (A) A normal flow–volume curve. (B) An
obstructive defect with characteristic concave shape during expiration. (C) The relatively unaffected shape but significantly decreased volume seen in restric­tive lung disease.
TLC RV
Obstructive
TLC RV
Restrictive
Obstructive
1
FVCFEV
Fig. 8.10 FEV1/FVC ratios. Normal = 4 L/5 L = 80%.
Obstructive FEV1/FVC = 1.2/3 = 40%. Restrictive FEV1/ FVC = 2.9/3.2 = 93%. FEV1, Forced Expiratory Volume in the first second; FVC, Forced Vital Capacity.
Regulation of Pulmonary Blood Flow
• Pulmonary arterioles do not appear to play an important role in the regulation of pulmonary blood ow, but the cali­bre of small alveolar vessels is altered by the PO2 and PCO2.
• Hypoxia (PO2) or hypercapnia (PCO2) result in con­striction of vessels and thus divert blood to areas that are better oxygenated; this is termed hypoxic pulmo­nary vasoconstriction (HPV).
• is is a local response and diers from other vascular beds in that the opposite response is usually seen (i.e. hypoxia causes vasodilatation).
Regional Variations in Pulmonary Blood Flow
• Perfusion pressure and resistance determine ow.
• Pressure in the pulmonary artery is low in comparison with the systemic circulation: 25/8 mmHg compared with 120/80 mmHg.
• Blood ow in the lung is determined by three pressures:
• hydrostatic pressure in the pulmonary arteries (PA)
• pressure in the pulmonary veins (PV)
• pressure of air in the alveoli.
• With these forces in mind the blood ow to the lung can be divided into three zones:
• zone 1: this is at the apex of the lung; the alveolar
pressure is similar to the PA pressure; smaller vessels will be compressed and resistance will be high. Blood ow is low in this zone
CHAPTER 8 Respiratory System
195
• zone 2: pressure in the PA is higher than the alveolar pressure; blood ow is better in this zone, increasing towards zone 3
• zone 3: PA pressure greatly exceeds the alveolar pres­sure and thus vessels are fully open. Blood ow is very good.
• e variations in regional blood ow are abolished on lying down.
Cardiac Output and Pulmonary Vascular Resistance
• During exercise the CO to the lungs increases but the pressure within the PA changes relatively little; this is due to two mechanisms which decrease resistance when CO increases:
• distension of vessels already open
• recruitment of additional vessels (at rest many capil-
laries are closed).
• e response to the increase in CO is passive.
Ventilation and Perfusion
• Ventilation and perfusion (V/Q) varies throughout the lung, depending on the height above or below the origin of the PA.
• e V/Q ratio expresses this variation:
• in alveoli that are ventilated but not perfused V/Q =
innity
• in alveoli that are perfused but not ventilated V/Q = 0
• at the apex V/Q = 3, thus indicating that the alveoli
are ventilated better than they are perfused
• at the base V/Q = 0.6, thus indicating that the alveoli
are perfused better than they are ventilated
• the ideal V/Q = 1 and is found approximately two-
thirds of the way up the chest
• the average V/Q ratio, assuming an alveolar ventila-
tion rate of 4.2 L/min, and a cardiac output of 5 L/min, would be 0.84.
Clinical Physiology
Pulmonary Embolus
• A pulmonary embolus results from a thrombus break­ing o from a thrombus formed in the large leg/pelvic veins; this clot then lodges in the pulmonary arteries.
• A pulmonary embolus can also occur with fat, amniotic uid, air or tumour fragments; these are all very rare.
• e eect of the embolus will depend on its size: clinical presentation varies from complete obstruction and sud­den death, to the insidious development of hypoxia due to numerous small emboli.
• e physiological changes associated with a pulmonary embolus include:
• increased pulmonary vascular resistance
• pulmonary hypertension
• increased right ventricle (RV) aerload (leading to RV dilatation and dysfunction)
• reduced le ventricle output
• impaired gas exchange, due to shunting of blood through non-perfused segments of lung
• decreased lung compliance, due to bleeding and loss of surfactant over the area aected by the embolus.
Pleural Effusion
• is refers to the abnormal presence of uid within the pleural cavity.
• e physiological consequences are similar to those of pneumothorax, i.e. hypoxia occurs as lung tissue is com­pressed by the uid and prevents normal gas exchange.
• e uid can be classied as a transudate or an exudate:
• an exudate has a high protein content (>30 g/L) and
is usually due to infection or cancer
• a transudate has a low protein content (<30 g/L) and
most commonly is due to le ventricular failure.
Pulmonary Oedema
• Pulmonary oedema is the abnormal accumulation of uid in the lung parenchyma.
• Starling’s law states that hydrostatic forces push uid out of the circulation and osmotic forces draw uid back.
• Normally the balance of hydrostatic and osmotic forces leads to 20–30 mL of excess uid in the lung intersti­tium; this is transported back to the circulation as lymph.
• Pulmonary oedema occurs in stages:
• interstitial oedema: this has little eect on respira-
tion, but will eventually overwhelm lymphatic recir­culation and lead to alveolar oedema
• alveolar oedema: as alveolar oedema develops, the
alveoli ll with uid; this increases surface tension and causes the alveoli to shrink
• airway oedema: as uid accumulation continues
then uid will begin to ll the airways; this presents as blood-tinged frothy sputum.
• e physiological eects of pulmonary oedema include:
• decreased lung compliance due to the reduction in
surface tension and alveolar shrinkage
• increased airway resistance: this can occur due to the
reduction in lung volume and uid lling the airways. Resistance is also due to reex bronchoconstriction.
• Alveolar oedema leads to a ventilation–perfusion mis­match as alveoli lled with uid are still perfused but not ventilated.
• Pulmonary vascular resistance increases due to hypoxic vasoconstriction and external compression from inter­stitial oedema.
196
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SECTION II Physiology
• ere are numerous causes of pulmonary oedema; these include:
• raised pulmonary hydrostatic pressure, the com-
monest cause, occurs with le ventricular failure – le atrial pressure rises and this is transmitted into the pulmonary circulation, resulting in increased pulmonary capillary pressure, and thus capillary hydrostatic pressure. is type of pulmonary oedema can also be seen with uid or transfusion overload
• increased pulmonary capillary permeability: this can
occur with endotoxic shock, irritant gases and adult respiratory distress syndrome (ARDS)
• blocked lymphatic drainage: this can occur in the face
of normal pulmonary hydrostatic pressures and nor­mal capillary permeability. e commonest cause is obstruction of lymphatics due to tumour cells. e nor­mal 20–30 mL of interstitial uid normally removed by lymphatics accumulates and leads to pulmonary oedema – it is called lymphangitis carcinomatosa
• high altitude: the exact cause is unclear, but is likely
to be due to hypoxic vasoconstriction leading to elevated pulmonary artery pressure and thus an increase in the hydrostatic pressure
• neurogenic: frequently seen in severe head injury
patients, it is thought to occur due to overactivity of the sympathetic nervous system.
Adult Respiratory Distress Syndrome
• ARDS is the pulmonary component of the systemic inammatory response syndrome (SIRS).
• It can be caused by direct (contusion, near drowning, aspiration, smoke inhalation) or indirect (trauma, sep­sis, pancreatitis) insults.
• Criteria for its diagnosis include:
• known cause
• acute onset of symptoms
• hypoxia refractory to O
• new, bilateral ‘uy’ inltrates on chest X-ray
2
• no evidence of cardiac failure (pulmonary artery
wedge pressure <18 mmHg).
• ARDS develops in two phases:
1. acute exudative: the insult (direct or indirect) leads
to neutrophil activation and the release of inam­matory mediators such as tumour necrosis factor (TNF), platelet activating factor (PAF), interleukin (IL)-1 and IL-6; there is also the release of prote­ases and toxic oxygen radicals that damage the lung parenchyma. is lung damage leads to increased capillary permeability and allows protein-rich exu­dates to ll the alveoli and form hyaline membranes. ere is thrombosis in alveolar capillaries and haemorrhage into the alveoli. is leads to alveolar
collapse and decreased surfactant production, lead­ing to decreased lung compliance
2. late organization: there is regeneration of type II pneumocytes; the hyaline membranes organize with pulmonary brosis, leading to interstitial brosis and obliteration of alveolar spaces and alveolar microvasculature.
Gas Diffusion and Exchange
Gas Diffusion
• ree factors aect the diusion of gases, both in the lungs and in the peripheral tissues:
• pressure gradient: gas ows from an area of high
pressure to an area of low pressure. is is usually referred to as the partial pressure
• diusion coecient: a measure of the ease with
which a gas can diuse. It is determined by its solu­bility in water and its molecular weight
• tissue factors: the tissue at the site of diusion should
have a large surface area and a short diusion dis­tance. e surface area of the lungs is about 70 m2 and the diusion distance is 0.2 µm.
• e diusion distance for oxygen consists of:
• pulmonary surfactant
• alveolar epithelium
• alveolar epithelium basement membrane (BM; oen
fused with capillary BM)
• pulmonary capillary endothelium.
Gas Exchange (Table 8.3)
• e exchange of gases in both peripheral tissues and alveoli relies on partial pressure gradients. In alveoli the gradient is between alveolar gas and pulmonary blood gas, while in the periphery the gradient is between cap­illary blood and metabolically active tissues.
• Room air: mixture of nitrogen and oxygen, water vapour (variable) and a tiny amount of carbon dioxide.
• Humidied air: inspired air becomes fully saturated with water; the partial pressure of water vapour is
6.3 kPa; the addition of water vapour leads to a decrease in the partial pressures of all other gases.
• Alveolar air: diers from room air due to the addition of water vapour and the constant removal of oxygen and carbon dioxide i.e. oxygen levels are lower and carbon dioxide levels are higher in comparison to room air.
Gas Transport (Fig. 8.11)
• Systemic venous blood is pumped into the pulmonary artery from the right ventricle. PO2 is 5.3 kPa and PCO2 is 6 kPa. Alveolar PO2 is 13.7 kPa and the PCO2 is 5.3 kPa.
• Following the principle of gases owing from areas of high partial pressure to low partial pressure, oxygen will
Pulmonary
Pulmonary
CHAPTER 8 Respiratory System
TABLE 8.3 Standard Values for Respiratory Gases
Gas Room Air (kPa) Humidified Air (kPa) Alveolar Air (kPa)
N
O
CO
2
2
2
79.79 74.83 75.6
21.17 19.87 13.7
0.04 0.04 5.3
H2O 0 6.3 6.3
Total 101 101 101
Oxygen transport
• Haemoglobin:
• consists of four peptide chains; two α and two β. Each peptide has a haem group which consists of a protoporphyrin ring surrounding a ferrous iron molecule (Fe2+)
• each haemoglobin (Hb) molecule can carry four oxygen molecules
• normal Hb values for a male and female are 15 g/dL and 13 g/dL, respectively. Each gram of Hb can carry
artery
PO PCO
2
2
= 13.7
= 5.3
CO
2
O
PO
PCO
Alveoli
2
PO
PCO
2
2
= 13.7
= 5.3
vein
= 5.3
2
= 6
2
1.34 mL of O2; therefore, O2-carrying capacity varies between 20 and 17.5 mL per 100 mL blood
Right heart
Left
heart
• the vast majority of O2 is transported via Hb; only a negligible amount is dissolved, approximately 0.225 per kPa of O2.
• Oxygen dissociation curve (Fig. 8.12):
• the oxygen dissociation curve illustrates the relation-
Systemic
vein
PO PCO
2
= 5.3
2
= 6
PO PCO
= 13
2
= 5.3
2
Systemic artery
ship between the partial pressure of O2 and the con­centration of O2 in the blood
• the characteristic shape of the curve reects the increasing ability of Hb to take up O2 following the binding of the rst molecule
Fig. 8.11 The gas exchange between the lungs and
tissues.
• the curve reaches a plateau at a PO2 of around 15–16 kPa
• a number of factors will alter the position of the curve. A right shi decreases oxygen anity and
diuse into the blood and carbon dioxide will diuse into the alveoli.
• Oxygenated blood is returned to the heart via the pul­monary veins and then to the le ventricle.
PO2 of systemic blood is slightly lower than pulmonary venous blood, due to the addition of deoxygenated blood from bronchial veins (13.7 kPa 13 kPa).
• e deoxygenated blood from bronchial veins is referred to as ‘shunting’; it describes the passage of blood through the lungs without coming into contact with ventilated alveoli. Other causes of shunt include:
• pneumonia (due to consolidation of lung parenchyma)
• atrial septal defect
• ventricular septal defect
• patent ductus arteriosus.
thus oxygen will be released at a higher partial pres­sure. A le shi increases oxygen anity
• a right shi is caused by:
temperature
2,3-diphosphoglycerate (2,3-DPG)
+
H
• the right shift of the dissociation curve is called the Bohr effect; the factors causing a right shift would be present in active tissues; the Bohr effect represents a mechanism to increase oxygen extraction
• anaemia does not aect the dissociation curve. e shape and position are the same; to see the eect of anaemia you would need to plot partial pressure against oxygen content.
197
198
100
Saturation (%)
13
100
O
saturation (%)
020406080 100 120
(mmHg)
Myoglobin
O
saturation (%)
)
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SECTION II Physiology
90
80
70
60
50
40
30
20
10
0
01234
A
75
50
2
25
0
0
246810 12 14 16
B
PCO
2,
2,3-DPG
TºC
[H+]
5
7
6
PaO2 (kPa)
PO
2
(kPa)
8910 11 12
100
75
50
2
25
0
0
C
0
Fetal Hb
Adult Hb
PO
2
2468
20 40 60 80 100120 (mmHg
10 12 14 16
(kPa)
Fig. 8.12 (A) Oxyhaemoglobin dissociation curve. (B) Factors that shift the oxyhaemoglobin curve to the right
and increase O2 dissociation. (C) Different O2 affinities for fetal haemoglobin and myoglobin in comparison with the O2 dissociation curve for adult Hb.
• Fetal haemoglobin and myoglobin:
• fetal haemoglobin (HbF) has dierent globin chains to adult Hb (two α and two γ); the change in globin chain results in a greater anity for O2 and allows the fetus to extract blood from the maternal circulation
• the curve for HbF is to the le of adult Hb, reecting the increased anity for O
• the curve for myoglobin lies further to the le; it acts as an oxygen storage molecule and only releases O2 when the partial pressure has fallen considerably
• the function of myoglobin is to provide additional O2 in muscles during periods of anaerobic respiration (i.e. during sustained contractions when blood ves­sels are compressed).
2
Carbon dioxide transport
• Carbon dioxide is transported in three main ways:
• carbamino groups: these are formed between CO2 and proteins or peptides. Most of these reactions are with the globin portions of haemoglobin, accounting for 20–30% of transported CO
• dissolved CO2 accounts for about 10% of the trans­ported CO
• HCO ported CO2. e CO2 diuses into the red blood cells
2
accounts for about 60–70% of the trans-
3
2
and reacts with water to form carbonic acid (a reac­tion catalysed by the enzyme carbonic anhydrase). e carbonic acid dissociates into H+ and HCO the H+ binds to haemoglobin and the HCO
diuses
3
;
3
30
60
Low (venous) PO
40 50 60 (mmHg)
55
blood)
–1
50
contents (ml 100 mL
2
45
CO
40
4
Y
High (arterial) PO
X
567
Fig. 8.13 The CO2 dissociation curve – Haldane effect.
X indicates CO2 content in systemic arterial blood (↑O2) and Y indicates CO2 content in venous blood (↓O2).
out of the cell into the plasma. To maintain cellular balance Cl− diuses into the red cell (chloride shi). is process is reversed in the alveoli, producing CO2 in preparation for expiration.
• e CO2 dissociation curve is for total CO2 and not one form; there are several dierences between it and the oxygen dissociation curve (Fig. 8.13):
• the solubility of CO2 is greater than oxygen
• the normal range of CO2 is much smaller: 5.3–6 kPa
compared with 5.3–13.3 kPa for oxygen
• blood cannot be saturated with CO2, therefore the
graph has no plateau phase.
• e CO2 dissociation curve is inuenced by the partial pressure of O2. Essentially the amount of carbon dioxide carried increases as the oxygen level falls; this eect is called the Haldane eect.
• e signicance of the Haldane eect is that as arte­rial blood (PCO2 5.3 kPa) passes through the capillary network (PCO2 6 kPa), the dissociation curve moves upwards and allows the increased uptake of CO2.
Regulation of Respiration
e body maintains the amount of PO2 and PCO2 at appro­priate levels through an interaction between neurological and chemical control mechanisms.
Neurological Regulation
• ere are a number of areas in the brain that exert dif­fering degrees of control on respiration. These areas include:
• medulla oblongata
Pco
8
CHAPTER 8 Respiratory System
199
• pons
2
• cerebral cortex
• limbic system and hypothalamus.
• Medulla oblongata: there are two groups of cells within the respiratory centre in the medulla:
• the inspiratory neurons: these demonstrate rhythmi-
2
cal ring of action potentials with intervening peri­ods of inactivity. ese action potentials stimulate the diaphragm and external intercostals to contract, and thus initiate inspiration. Expiration occurs dur­ing the intervening pauses of inactivity
• the expiratory neurons: these neurons are usually
2
(kPa)
inactive during normal quiet respiration; however, during periods of exercise or increased respiration they re action potentials during the inactive period of the inspiratory neurons to stimulate the internal intercostals and abdominal muscles to contract, and thus aid expiration.
• Pons: there are two areas within the pons; they are not essential for respiration, but can inuence the pattern of breathing:
• apneustic centre: this is located in the lower pons;
it tends to prolong inspiration and results in short expiratory eorts
• pneumotaxic centre: this is located in the upper
pons; it tends to inhibit the inspiratory neurons and shortens inspiration.
• Cerebral cortex: this can override the neurons within the medulla and increase ventilation (hyperventilate) or hold the breath.
• Limbic system and hypothalamus: in extreme states of emotion, such as fear or anger, these areas may inu­ence the respiratory pattern.
Chemical Regulation
• e rhythmical ring of neurons in the medulla is regu­lated by the input of a number of chemoreceptors, which monitor changes in chemical factors and then signal the medulla to increase or decrease the respiratory rate to normalize the detected chemical change.
• ese chemoreceptors monitor changes in the following:
• arterial PCO
• arterial pH
2
• arterial PO2.
• ese chemoreceptors can be further subdivided into:
• central chemoreceptors
• peripheral chemoreceptors.
• Central chemoreceptors:
• situated in the CNS, close to the respiratory centre in
the medulla
• particularly sensitive to changes in the arterial
PCO
2
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SECTION II Physiology
• CO2 diuses from the blood into the brain and reacts with water to produce H+ and causes the pH to fall, thus directly stimulating the chemoreceptors
• any elevation in CO2 leads to a central acidosis that stimulates the chemoreceptors and leads to an increased respiratory rate in order to blow o the excess CO2. e opposite eect is seen with low lev­els of CO
• central chemoreceptors are the main determinant of
2
respiration, as the level of CO2 is the most important stimulus to respiration.
• Peripheral chemoreceptors:
• located in the carotid bodies, close to the bifurca­tion of the common carotid and in the aortic bodies, which lie along the aortic arch
• less important than the central chemoreceptors
• they respond to changes in arterial pH and to low levels of PO2; the response to pH is of secondary importance to respiratory control but does allow compensation for acid–base disturbances
• for instance, a fall in arterial pH due to a metabolic acidosis will stimulate respiration and thus will lower the level of CO2 and favour an increase in pH back towards normal. e opposite eect is seen with an alkalosis
• the response to low O2 only comes into eect when levels are abnormally low, i.e. PO2 8 kPa or less
• these receptors can become important in severe longstanding lung disease with persistently elevated levels of CO2. Patients may become accustomed and lose the controlling inuence of CO2. ey therefore rely on the low level of O2 to stimulate respiration. is is called hypoxic drive.
• ere are several other factors which may inuence respiration:
• Hering–Breuer reex: this reex prevents over-ina-
tion of the lungs. Stretch receptors in the lung send inhibitory signals via the vagus. Only signicant at high tidal volumes (>1.5 L)
• ‘J’ receptors: these receptors lie in the alveoli in close
association with the capillaries. eir function is unclear but injection of chemicals into the pulmo­nary circulation triggers these receptors and causes a marked inhibition of inspiration
• irritant receptors: lie in the epithelia lining the air-
ways; they respond to noxious gases and cause bron­chospasm and inhibition of inspiration
• vasomotor centre: low blood pressure detected by
baroreceptors results in an increase in the ventilatory rate. An increase in blood pressure has the opposite eect.
Hypoxia and Respiratory Failure
Hypoxia and Hypoxaemia
• Hypoxia: a deciency of oxygen in the tissues.
• Hypoxaemia: reduction in the concentration of oxygen in the arterial blood.
• ere are four types of hypoxia:
1. Hypoxic hypoxia: results from a low arterial PO2;
examples include:
• high altitude
• pulmonary embolism
• hypoventilation
• lung brosis
• pulmonary oedema.
2. Anaemic hypoxia: a decrease in the amount of hae-
moglobin and thus a decrease in oxygen content of arterial blood; examples include:
• haemorrhage
• decreased red cell production
• increased red cell destruction
• carbon monoxide poisoning.
3. Stagnant hypoxia: due to low blood ow; examples
include:
• vasoconstriction
• decreased cardiac output: due to the low blood ow there is increased extraction of oxygen from the blood; this leads to very low venous oxygen and produces peripheral cyanosis.
4. Histotoxic hypoxia: poisoning of the enzymes involved in cellular respiration. Oxygen is available but cannot be utilized; the main example is cyanide poisoning.
• ere are ve main causes of hypoxaemia:
1. Hypoventilation, accompanied by PaCO2; oxygen therapy can improve the hypoxaemia; common causes of hypoventilation include:
• central depression of respiratory drive, e.g. drugs
• trauma, i.e. cervical cord injury
• neuromuscular disorders, e.g. myasthenia gravis
• chest wall deformity.
2. Impaired diusion: PaCO2 is usually normal due to its increased solubility; oxygen therapy can also improve the hypoxaemia. Causes of impaired diu­sion include:
• asbestosis
• sarcoidosis
• ARDS.
3. Shunt (see Gas Transport section): PaCO2 is usually normal, but unlike other causes of hypoxaemia the administration of oxygen will not raise the PaO2; this